U.S. patent number 10,312,833 [Application Number 15/305,314] was granted by the patent office on 2019-06-04 for power generator.
This patent grant is currently assigned to MITSUMI ELECTRIC CO., LTD. The grantee listed for this patent is MITSUMI ELECTRIC CO., LTD.. Invention is credited to Kenichi Furukawa, Takayuki Numakunai.
United States Patent |
10,312,833 |
Furukawa , et al. |
June 4, 2019 |
Power generator
Abstract
A power generator 1 includes a magnetostrictive rod 2 through
which lines of magnetic force pass in an axial direction thereof, a
beam member 73 having a function of generating stress in the
magnetostrictive rod 2, and a coil 3 arranged so that the lines of
magnetic force pass inside the coil 3 in an axial direction of the
coil 3. The beam member 73 is arranged along the magnetostrictive
rod 2 and configured to allow one end portion and the other end
portion of the magnetostrictive rod 2 to approach to each other to
generate compressive stress in the magnetostrictive rod 2. Further,
in the power generator 1, it is preferable that a gap between the
beam member 73 and the magnetostrictive rod 2 on the side of the
one end portion of the magnetostrictive rod 2 is larger than a gap
between the beam member 73 and the magnetostrictive rod 2 on the
side of the other one end portion of the magnetostrictive rod 2 in
a side view.
Inventors: |
Furukawa; Kenichi (Sagamihara,
JP), Numakunai; Takayuki (Tama, JP) |
Applicant: |
Name |
City |
State |
Country |
Type |
MITSUMI ELECTRIC CO., LTD. |
Tokyo |
N/A |
JP |
|
|
Assignee: |
MITSUMI ELECTRIC CO., LTD
(Tokyo, JP)
|
Family
ID: |
54332157 |
Appl.
No.: |
15/305,314 |
Filed: |
February 19, 2015 |
PCT
Filed: |
February 19, 2015 |
PCT No.: |
PCT/JP2015/054671 |
371(c)(1),(2),(4) Date: |
October 19, 2016 |
PCT
Pub. No.: |
WO2015/162984 |
PCT
Pub. Date: |
October 29, 2015 |
Prior Publication Data
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|
|
Document
Identifier |
Publication Date |
|
US 20170040912 A1 |
Feb 9, 2017 |
|
Foreign Application Priority Data
|
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|
|
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Apr 23, 2014 [JP] |
|
|
2014-088801 |
|
Current U.S.
Class: |
1/1 |
Current CPC
Class: |
H02K
3/28 (20130101); H01L 41/125 (20130101); H02N
2/18 (20130101); H02K 1/34 (20130101) |
Current International
Class: |
H01L
41/12 (20060101); H02K 3/28 (20060101); H02N
2/18 (20060101); H02K 1/34 (20060101) |
Field of
Search: |
;310/26 |
References Cited
[Referenced By]
U.S. Patent Documents
Foreign Patent Documents
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|
|
|
|
2013-208026 |
|
Oct 2013 |
|
JP |
|
2013-208028 |
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Oct 2013 |
|
JP |
|
2014-033507 |
|
Feb 2014 |
|
JP |
|
2014132812 |
|
Jul 2014 |
|
JP |
|
2015122855 |
|
Jul 2015 |
|
JP |
|
2011158473 |
|
Dec 2011 |
|
WO |
|
Other References
International Search Report, PCT/JP2015/054671, dated May 19, 2015,
1 page. cited by applicant.
|
Primary Examiner: Luks; Jeremy A
Attorney, Agent or Firm: Miller Nash Graham & Dunn
LLP
Claims
What is claimed is:
1. A power generator comprising: a magnetostrictive rod through
which lines of magnetic force pass in an axial direction thereof,
the magnetostrictive rod formed of a magnetostrictive material; a
coil arranged so that the lines of magnetic force pass inside the
coil in an axial direction of the coil whereby a voltage is
generated in the coil due to variation of density of the lines of
magnetic force; and a bias stress generating mechanism for
generating compressive stress in the magnetostrictive rod in a
natural state, wherein the magnetostrictive rod has one end portion
and the other end portion, and wherein the power generator is
configured to generate the voltage in the coil due to the variation
of the density of the lines of magnetic force when the other end
portion of the magnetostrictive rod is displaced with respect to
the one end portion of the magnetostrictive rod in a direction
substantially perpendicular to the axial direction of the
magnetostrictive rod to expand and contract the magnetostrictive
rod, wherein the bias stress generating mechanism includes a beam
member which is arranged along the magnetostrictive rod and allows
the one end portion and the other end portion of the
magnetostrictive rod to approach to each other to generate the
compressive stress in the magnetostrictive rod.
2. The power generator as claimed in claim 1, wherein a gap between
the beam member and the magnetostrictive rod on the side of the
other end portion of the magnetostrictive rod is smaller than a gap
between the beam member and the magnetostrictive rod on the side of
the one end portion of the magnetostrictive rod in a side view.
3. The power generator as claimed in claim 1, wherein the beam
member is formed of a non-magnetic material.
4. The power generator as claimed in claim 1, wherein the
magnetostrictive rod includes two or more of magnetostrictive rods
arranged side by side, and wherein the two or more of
magnetostrictive rods are arranged so as not to overlap with the
beam member in a planar view.
5. The power generator as claimed in claim 4, wherein the beam
member is arranged between the magnetostrictive rods in the planar
view.
6. The power generator as claimed in claim 1, wherein the bias
stress generating mechanism further includes a magnetic member
provided on the side of the other end portion of the
magnetostrictive rod and a magnet for attracting the magnetic
member so as to generate the compressive stress in the
magnetostrictive rod.
7. The power generator as claimed in claim 1, further comprising: a
first block body including a receiving portion for receiving the
one end portion of the magnetostrictive rod, the first block body
formed of a magnetic material; and a second block body including a
receiving portion for receiving the other end portion of the
magnetostrictive rod, the second block body formed of a magnetic
material.
8. The power generator as claimed in claim 1, wherein the coil is
wound around the magnetostrictive rod.
Description
FIELD OF THE INVENTION
The present invention relates to a power generator.
BACKGROUND ART
In recent years, there has been developed a power generator which
can generate electric power by utilizing variation of magnetic
permeability of a magnetostrictive rod formed of a magnetostrictive
material (for example, see patent document 1).
For example, this power generator includes a pair of
magnetostrictive rods arranged side by side, two connecting yokes
for respectively connecting one end portions and the other end
portions of the pair of magnetostrictive rods with each other,
coils arranged so as to respectively surround the magnetostrictive
rods, two permanent magnets respectively arranged on the two
connecting yokes to apply a bias magnetic field to the
magnetostrictive rods and a back yoke. The pair of magnetostrictive
rods serve as beams facing each other. When external force is
applied to one of the connecting yokes in a direction perpendicular
to each axial direction of the pair of the magnetostrictive rods,
one of the magnetostrictive rods is deformed so as to be expanded
and the other one of the magnetostrictive rods is deformed so as to
be contracted. At this time, magnetic permeability of each
magnetostrictive rod 2 varies. This variation of the magnetic
permeability of each magnetostrictive rod 2 leads to variation of
density of lines of magnetic force (magnetic flux density) passing
through the magnetostrictive rods (that is density of the lines of
magnetic force passing through the coils), thereby generating a
voltage in the coils.
Generally, the magnetostrictive rod as described above has
characteristics that a variation amount (decreasing amount) of the
magnetic flux density (magnetic permeability) caused by generation
of compressive stress is large while a variation amount (increasing
amount) of the magnetic flux density (magnetic permeability) caused
by generation of tensile stress is small. Thus, it is difficult to
sufficiently vary the magnetic flux density of each of the
magnetostrictive rods even if the external power is applied to the
power generator to alternately generate the tensile stress and the
compressive stress in each of the magnetostrictive rods because the
variation amount of the magnetic flux density caused by the tensile
stress is small.
Further, the variation amount of the magnetic flux density of each
of the magnetostrictive rods is affected by an intensity of the
bias magnetic field applied to the magnetostrictive rods.
Generally, the variation amount of the magnetic flux density
decreases as the intensity of the applied bias magnetic field
increases.
Thus, in the power generator disclosed in the patent document 1, if
the intensity of the bias magnetic field applied to the
magnetostrictive rods is large, it is impossible to sufficiently
increase the variation amount of the magnetic flux density of each
of the magnetostrictive rods (specifically, it is required to
increase the variation amount of the magnetic flux density to about
1 T) without significantly increasing the external force applied to
the magnetostrictive rods to sufficiently increase magnitudes of
the tensile stress and the compressive stress caused in each of the
magnetostrictive rods. Thus, if the intensity of the bias magnetic
field applied to the magnetostrictive rods is large, it is
difficult for the power generator disclosed in the patent document
1 to efficiently generate the electric power.
RELATED ART
Patent Document
Patent document 1: WO 2011/158473
SUMMARY OF THE INVENTION
Problems to be Solved by the Invention
The present invention has been made in view of the problems
mentioned above. Accordingly, it is an object of the present
invention to provide a power generator which can efficiently
generate electric power in a wide range of a bias magnetic field.
Further, it is also an object of the present invention to provide a
power generator whose degree of freedom for design is high.
Means for Solving the Problems
The above objects are achieved by the present inventions defined in
the following (1) to (13).
(1) A power generator comprising:
a magnetostrictive rod through which lines of magnetic force pass
in an axial direction thereof, the magnetostrictive rod formed of a
magnetostrictive material;
a coil arranged so that the lines of magnetic force pass inside the
coil in an axial direction of the coil whereby a voltage is
generated in the coil due to variation of density of the lines of
magnetic force; and
a bias stress generating mechanism for generating compressive
stress in the magnetostrictive rod in a natural state,
wherein the magnetostrictive rod has one end portion and the other
end portion, and
wherein the power generator is configured to generate the voltage
in the coil due to the variation of the density of the lines of
magnetic force when the other end portion of the magnetostrictive
rod is displaced with respect to the one end portion of the
magnetostrictive rod in a direction substantially perpendicular to
the axial direction of the magnetostrictive rod to expand and
contract the magnetostrictive rod.
(2) The power generator according to the above (1), wherein the
bias stress generating mechanism includes a beam member which is
arranged along the magnetostrictive rod and allows the one end
portion and the other end portion of the magnetostrictive rod to
approach to each other to generate the compressive stress in the
magnetostrictive rod.
(3) The power generator according to the above (2), wherein a gap
between the beam member and the magnetostrictive rod on the side of
the other end portion of the magnetostrictive rod is smaller than a
gap between the beam member and the magnetostrictive rod on the
side of the one end portion of the magnetostrictive rod in a side
view.
(4) The power generator according to the above (2) or (3), wherein
the beam member is formed of a non-magnetic material.
(5) The power generator according to any one of the above (2) to
(4), wherein the magnetostrictive rod includes two or more of
magnetostrictive rods arranged side by side, and
wherein the two or more of magnetostrictive rods are arranged so as
not to overlap with the beam member in a planar view.
(6) The power generator according to the above (5), wherein the
beam member is arranged between the magnetostrictive rods in the
planar view.
(7) The power generator according to any one of the above (1) to
(6), wherein the bias stress generating mechanism includes an
elastic member for generating the compressive stress in the
magnetostrictive rod.
(8) The power generator according to the above (7), wherein the
elastic member includes a coil spring for pushing or pulling the
other end portion of the magnetostrictive rod in a displacement
direction in which the magnetostrictive rod can be displaced to
generate the compressive stress in the magnetostrictive rod.
(9) The power generator according to the above (7) or (8), wherein
the elastic member includes a coil spring for pulling the
magnetostrictive rod in a direction in which the one end portion
and the other end portion of the magnetostrictive rod approach to
each other.
(10) The power generator according to the above (7) or (8), wherein
the elastic member includes a wire for pulling the magnetostrictive
rod in a direction in which the one end portion and the other end
portion of the magnetostrictive rod approach to each other.
(11) The power generator according to any one of the above (1) to
(10), wherein the bias stress generating mechanism further includes
a magnetic member provided on the side of the other end portion of
the magnetostrictive rod and a magnet for attracting the magnetic
member so as to generate the compressive stress in the
magnetostrictive rod.
(12) The power generator according to any one of the above (1) to
(11), further comprising:
a first block body including a receiving portion for receiving the
one end portion of the magnetostrictive rod, the first block body
formed of a magnetic material; and
a second block body including a receiving portion for receiving the
other end portion of the magnetostrictive rod, the second block
body formed of a magnetic material.
(13) The power generator according to any one of the above (1) to
(12), wherein the coil is wound around the magnetostrictive
rod.
Effects of the Invention
According to the present invention, since the compressive stress
(contraction stress) is generated in the magnetostrictive rod in
the natural state (that is a state that external force is not
applied to the power generator), the magnetic permeability of the
magnetostrictive rod is lower than the case where the stress does
not occur in the magnetostrictive rod. Thus, in this power
generator, it is possible to increase the variation amount of the
magnetic flux density caused by the generation of the tensile
stress (stretching stress) in the magnetostrictive rod and
sufficiently increase the variation amount of the magnetic flux
density in the magnetostrictive rod when the tensile stress and the
compressive stress are alternately generated in the
magnetostrictive rod.
Further, generally, the variation amount of the magnetic flux
density in the magnetostrictive rod increases until the intensity
of the applied bias magnetic field reaches to a predetermined value
(optimum value) and decreases as this intensity increases over the
optimum value. According to the present invention, even in the case
where the intensity of the bias magnetic field applied to the
magnetostrictive rod is larger than the optimum value, it is
possible to sufficiently increase the variation amount of the
magnetic flux density in the magnetostrictive rod. Namely, it is
possible to sufficiently increase the variation amount of the
magnetic flux density in the magnetostrictive rod in a wide range
of intensities of the bias magnetic field. As a result, it is
possible to provide a power generator which can efficiently
generate the electric power in a wide range of the bias magnetic
field. Further, it is also possible to provide a power generator
whose degree of freedom for design is high.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a perspective view showing a first embodiment of a power
generator of the present invention.
FIG. 2 is an exploded perspective view of the power generator shown
in FIG. 1.
FIG. 3(a) is a right-side view of the power generator shown in FIG.
1. FIG. 3(b) is a view showing a state that coils are removed from
magnetostrictive rods shown in FIG. 3(a).
FIG. 4 is a planar view of the power generator shown in FIG. 1.
FIG. 5 is a front view of the power generator shown in FIG. 1.
FIG. 6(a) is a side view showing a state that the power generator
(with the coils being omitted) shown in FIG. 1 is attached to a
vibrating body. FIG. 6(b) is a view showing a state that external
force is applied to a tip end portion of the power generator shown
in FIG. 6(a) in the lower direction.
Each of FIGS. 7(a) and 7(b) is a graph showing a relationship
between magnetic flux density (B) and a bias magnetic field (H)
applied to a magnetostrictive rod formed of a magnetostrictive
material containing an iron-gallium based alloy as a main component
thereof depending on stress generated in the magnetostrictive rod.
FIG. 7(c) is a graph showing a relationship between a variation
amount of the magnetic flux density (.DELTA.B) and the bias
magnetic field (H) applied to the magnetostrictive rod depending on
the stress generated in the magnetostrictive rod. In this graph, a
state in that the stress does not occur in the magnetostrictive rod
is utilized as a reference. FIG. 7(d) is a graph showing the
relationship between the variation amount of the magnetic flux
density (.DELTA.B) and the bias magnetic field (H) applied to the
magnetostrictive rod depending on the stress generated in the
magnetostrictive rod. In this graph, a state that compressive
stress of 14.15 MPa occurs in the magnetostrictive rod is utilized
as a reference.
FIG. 8 is a side view schematically showing a state that external
force in the lower direction is applied to a tip end portion of one
rod member (one beam) whose base end portion is fixed to a
housing.
FIG. 9 is a side view schematically showing a state that external
force in the lower direction is applied to tip end portions of a
pair of beams (parallel beams) parallel arranged so as to face each
other whose base end portions are fixed to the housing.
FIG. 10 is a view schematically showing stress (tensile stress and
compressive stress) generated in the pair of parallel beams when
the external force is applied to the tip end portions of the pair
of parallel beams.
FIG. 11 is a planar view showing another configuration example of
the power generator of the first embodiment of the present
invention.
FIG. 12(a) is a right-side view (with the coils being omitted) for
explaining a state before a connecting portion is attached to each
block body in the other configuration example of the power
generator of the first embodiment of the present invention. FIG.
12(b) is a right-side view (with the coils being omitted) of the
other configuration example of the power generator of the first
embodiment of the present invention.
FIG. 13 is a side view showing a second embodiment of the power
generator of the present invention.
FIG. 14 is a side view showing another configuration example of the
power generator of the second embodiment of the present
invention.
FIG. 15 is a side view showing a third embodiment of the power
generator of the present invention.
FIG. 16 is a perspective view showing a fourth embodiment of the
power generator of the present invention.
FIG. 17 is a side view of the power generator shown in FIG. 16.
FIG. 18 is a side view showing another configuration example of the
power generator of the fourth embodiment of the present
invention.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
Hereinafter, description will be given to a power generator of the
present invention with reference to preferred embodiments shown in
the accompanying drawings.
First Embodiment
First, description will be given to a first embodiment of the power
generator of the present invention.
FIG. 1 is a perspective view showing the first embodiment of the
power generator of the present invention. FIG. 2 is an exploded
perspective view of the power generator shown in FIG. 1. FIG. 3(a)
is a right-side view of the power generator shown in FIG. 1. FIG.
3(b) is a view showing a state that coils are removed from
magnetostrictive rods shown in FIG. 3(a). FIG. 4 is a planar view
of the power generator shown in FIG. 1. FIG. 5 is a front view of
the power generator shown in FIG. 1. FIG. 6(a) is a side view
showing a state that the power generator (with the coils being
omitted) shown in FIG. 1 is attached to a vibrating body. FIG. 6(b)
is a view showing a state that external force is applied to a tip
end portion of the power generator shown in FIG. 6(a) in the lower
direction.
Hereinafter, an upper side in each of FIGS. 1, 2, 3(a), 3(b), 5,
6(a) and 6(b) and a front side of the paper in FIG. 4 are referred
to as "upper" or "upper side" and a lower side in each of FIGS. 1,
2, 3(a), 3(b), 5, 6(a) and 6(b) and a rear side of the paper in
FIG. 4 are referred to as "lower" or "lower side". Further, a right
and rear side of the paper in each of FIGS. 1 and 2 and a right
side of each of FIGS. 3(a), 3(b), 4, 6(a) and 6(b) are referred to
as "tip end side" and a left and front side of the paper in each of
FIGS. 1 and 2 and a left side in each of FIGS. 3(a), 3(b), 4, 6(a)
and 6(b) are referred to as "base end side".
A power generator 1 shown in FIGS. 1 and 2 includes two
magnetostrictive rods 2 through which lines of magnetic force pass
in an axial direction thereof, coils 3 arranged so that the lines
of magnetic force pass inside the coils 3 in an axial direction of
each of the coils 3, and a beam member 73 having a function of
generating stress in each of the magnetostrictive rods 2. Each of
the magnetostrictive rods 2 includes a base end portion (one end
portion) 21 and a tip end portion (the other end portion) 22. In
this power generator 1, the tip end portion 22 of each of the
magnetostrictive rods 2 is displaced with respect to the base end
portion 21 of each of the magnetostrictive rods 2 in a direction
substantially perpendicular to an axial direction of each of the
magnetostrictive rods 2 (the vertical direction in FIG. 1) to
expand and contract each of the magnetostrictive rods 2. At this
time, magnetic permeability of each of the magnetostrictive rods 2
varies due to an inverse magnetostrictive effect. This variation of
the magnetic permeability of each magnetostrictive rod 2 leads to
variation of density of the lines of magnetic force passing through
the magnetostrictive rods 2 (density of the lines of magnetic force
passing through the coils 3), thereby generating a voltage in the
coils 3.
Hereinafter, description will be given to each component of the
power generator 1.
(Magnetostrictive Rod 2)
As shown in FIGS. 1 and 2, the power generator 1 of this embodiment
includes the two magnetostrictive rods 2 arranged side by side.
Each of the magnetostrictive rods 2 is formed of a magnetostrictive
material and arranged so that a direction in which magnetization is
easily generated (an easy magnetization direction) coincides with
the axial direction thereof. In this embodiment, each of the
magnetostrictive rods 2 has an elongated plate-like shape so that
the lines of magnetic force pass through each of the
magnetostrictive rods 2 in the axial direction thereof.
A thickness (cross-sectional area) of each of the magnetostrictive
rods 2 is substantially constant along the axial direction thereof.
An average thickness of each of the magnetostrictive rods 2 is not
particularly limited to a specific value, but is preferably in the
range of about 0.3 to 10 mm, and more preferably in the range of
about 0.5 to 5 mm. Further, an average value of the cross-sectional
area of each of the magnetostrictive rods 2 is preferably in the
range of about 0.2 to 200 mm.sup.2, and more preferably in the
range of about 0.5 to 50 mm.sup.2. With such a configuration, it is
possible to reliably pass the lines of magnetic force through the
magnetostrictive rods 2 in the axial direction thereof.
A Young's modulus of the magnetostrictive material is preferably in
the range of about 40 to 100 GPa, more preferably in the range of
about 50 to 90 GPa, and even more preferably in the range of about
60 to 80 GPa. By forming the magnetostrictive rods 2 with the
magnetostrictive material having the above Young's modulus, it is
possible to expand and contract the magnetostrictive rods 2 more
drastically. Since this allows the magnetic permeability of each of
the magnetostrictive rods 2 to vary more drastically, it is
possible to more improve power generation efficiency of the power
generator 1 (the coils 3).
The magnetostrictive material having the above Young's modulus is
not particularly limited to a specific kind. Examples of such a
magnetostrictive material include an iron-gallium based alloy, an
iron-cobalt based alloy, an iron-nickel based alloy and a
combination of two or more of these materials. Among them, a
magnetostrictive material containing an iron-gallium based alloy
(having a Young's modulus of about 70 GPa) as a main component
thereof is preferably used. A Young's modulus of the
magnetostrictive material containing the iron-gallium based alloy
as the main component thereof can be easily adjusted to fall within
the above range.
Further, it is preferable that the magnetostrictive material
described above contains at least one of rare-earth metals such as
Y, Pr, Sm, Tb, Dy, Ho, Er and Tm. By using the magnetostrictive
material containing at least one rare-earth metal mentioned above,
it is possible to more increase the variation of the magnetic
permeability of each of the magnetostrictive rods 2.
The coils 3 are respectively wound around outer peripheries of the
magnetostrictive rods 2 (arranged on the outer peripheral sides of
the magnetostrictive rods 2) so as to respectively surround a
portion of each magnetostrictive rod 2 except for both end portions
21, 22 of the magnetostrictive rod 2.
(Coil 3)
Each of the coils 3 is formed by winding a wire 31 around each
magnetostrictive rod 2. With such a configuration, the coils 3 are
arranged so that the lines of magnetic force passing through the
magnetostrictive rods 2 pass inside the coils 3 (inner cavities of
the coils 3) in an axial direction of the coils 3 (in this
embodiment, the axial direction of the coils 3 is equivalent to the
axial direction of the magnetostrictive rods 2). Due to the
variation of the magnetic permeability of each of the
magnetostrictive rods 2, that is, due to the variation of the
density of the lines of magnetic force (magnetic flux density)
passing through the magnetostrictive rods 2, the voltage is
generated in the coils 3.
In the power generator 1 of this embodiment, the magnetostrictive
rods 2 are arranged side by side in not a thickness direction
thereof but a width direction thereof. Thus, it is possible to make
a gap between the magnetostrictive rods 2 larger at the time of
designing the power generator 1. Therefore, it is possible to
sufficiently ensure spaces for the coils 3 wound around the
magnetostrictive rods 2, thereby increasing a winding number of
each of the coils 3 even if a wire 31 having a relatively large
cross-sectional area (diameter) is used for forming each of the
coils 3. Since the wire 31 having a large diameter has a small
resistance value (small load impedance), it is possible to allow
electric current to flow in the coils 3 efficiently, thereby
efficiently utilizing the voltage generated in the coils 3.
The voltage .epsilon. generated in the coils 3 can be expressed by
the following formula (1) based on the variation of the magnetic
flux density of each of the magnetostrictive rods 2.
.epsilon.=N.times..DELTA.B/.DELTA.T (1)
(wherein "N" is the winding number of the wire 31, ".DELTA.B" is a
variation amount of the magnetic flux passing in the inner cavities
of the coils 3 and ".DELTA.T" is a variation amount of time.)
As is clear from the above formula (1), the voltage .epsilon.
generated in each of the coils 3 is proportional to the winding
number of the wire 31 and the variation amount of the magnetic flux
density of each of the magnetostrictive rods 2 (.DELTA.B/.DELTA.T).
Thus, it is possible to improve the power generation efficiency of
the power generator 1 by increasing the winding number of the wire
31.
The wire 31 is not particularly limited to a specific type.
Examples of the wire 31 include a wire obtained by covering a
copper base line with an insulating layer, a wire obtained by
covering a copper base line with an insulating layer to which an
adhesive (fusion) function is imparted and a combination of two or
more of these wires.
The winding number of the wire 31 is not particularly limited to a
specific value, but is preferably in the range of about 1000 to
10000, and more preferably in the range of about 2000 to 9000. With
such a configuration, it is possible to more increase the voltage
generated in each of the coils 3.
Further, the cross-sectional area of the wire 31 is not
particularly limited to a specific value, but is preferably in the
range of about 5.times.10.sup.-4 to 0.15 mm.sup.2, and more
preferably in the range of about 2.times.10.sup.-3 to 0.08
mm.sup.2. Since the wire 31 with such a cross-sectional area of the
above range has a sufficiently small resistance value, it is
possible to efficiently output the electric current flowing in each
of the coils 3 to the outside with the generated voltage. As a
result, it is possible to improve the power generation efficiency
of the power generator 1.
A cross-sectional shape of the wire 31 may be any shape. Examples
of the cross-sectional shape of the wire 31 include a polygonal
shape such as a triangular shape, a square shape, a rectangular
shape and a hexagonal shape; a circular shape and an elliptical
shape.
Although this matter is not shown in the drawings, both end
portions of the wire 31 of each of the coils 3 are connected to an
electric circuit such as a wireless device (wireless communication
device). With this configuration, it is possible to utilize the
voltage (electric power) generated in the coils 3 for the electric
circuit.
First block bodies 4 are provided on the base end side of each
magnetostrictive rod 2.
(First Block Body 4)
The first block bodies 4 serve as a fixing portion for fixing the
power generator 1 to a vibrating body generating vibration. By
fixing the power generator 1 to the vibrating body through the
first block bodies 4, each of the magnetostrictive rods 2 is
supported in a cantilevered state that the base end portions 21
thereof serve as fixed end portions and the tip end portions 22
thereof serve as movable end portions. Examples of the vibrating
body to which the first block bodies 4 are fixedly attached include
a variety of vibrating bodies such as an air-conditioning duct.
Concrete examples of the vibrating body will be described
later.
As shown in FIGS. 1 and 2, each of the first block bodies 4 has a
tall block body 41 provided on the tip end side and a short block
body 42 shorter (thinner) than this tall block body 41. An external
shape of each of the first block bodies 4 is a step-wise shape
(multi-level shape).
A slit 411 is formed on a substantially central portion of the tall
block body 41 in a thickness direction thereof along a width
direction of the tall block body 41. The base end portion 21 of the
magnetostrictive rod 2 is inserted (received) into this slit 411.
Further, a pair of female screw portions 412 are formed in both end
portions of the tall block body 41 in the width direction thereof
so as to pass through the tall block body 41 in the thickness
direction thereof. Male screws 43 are respectively screwed into the
female screw portions 412.
A pair of female screw portions 421 are formed in both end portions
of the short block body 42 in a width direction thereof so as to
pass through the short block body 42 in a thickness direction
thereof. Male screws 44 are respectively screwed into the female
screw portions 421. By screwing these male screws 44 into a housing
and the like through the female screw portions 421, it is possible
to fix the first block bodies 4 to the housing.
Further, a groove 422 is formed on a lower surface of the short
block body 42 so as to extend in the width direction of the short
block body 42. Thus, since each of the first block bodies 4 is
fixed to the vibrating body through two portions (that is a portion
on the base end side (the short block body 42) and a portion on the
tip end side (the tall block body 41) facing each other through the
groove 422), each of the first block bodies 4 is configured so as
to be easily deformed (bent) in the vicinity of the groove 422.
Therefore, it is possible to efficiently transfer the vibration of
the vibrating body to the tip end portions 22 of the
magnetostrictive rods 2 (second block bodies 5) through the first
block bodies 4. As a result, it is possible to efficiently generate
the tensile stress (stretching stress) or the compressive stress
(contraction stress) in the magnetostrictive rods 2.
On the other hand, the second block bodies 5 are provided on the
tip end side of the magnetostrictive rods 2.
(Second Block Body 5)
Each of the second block bodies 5 serves as a weight for applying
external force or vibration to the magnetostrictive rods 2. When
the vibrating body vibrates, external force or vibration in the
vertical direction is applied to the second block bodies 5. By
applying the external force or the vibration to the second block
bodies 5, the tip end portions 22 of the magnetostrictive rods 2
begin reciprocating motion in the vertical direction in the
cantilevered state that the base end portions 21 of the
magnetostrictive rods 2 serve as the fixed end portions and the tip
end portions 22 of the magnetostrictive rods 2 serve as the movable
end portions. Namely, the tip end portions 22 of the
magnetostrictive rods 2 are relatively displaced with respect to
the base end portions 21 of the magnetostrictive rods 2.
As shown in FIGS. 1 and 2, each of the second block bodies 5 has a
substantially rectangular parallelepiped shape. A multi-level
portion 55 is formed on each of the second block bodies 5 so as to
be a step-wise shape (multi-level shape) having steps whose step on
the base end side is lower than a step on the tip end side by two
levels. The multi-level portion 55 has a first level surface 551
which is provided on the base end side and on which the tip end
portion 22 of the magnetostrictive rod 2 is to be placed (received)
and a second level surface 552 provided on the tip end side of the
first level surface 551 and being higher than the first level
surface 551 by one level. In this regard, a height from the second
level surface 522 to the first level surface 551 of the second
block body 5 is set so as to be substantially equal to a thickness
of the tip end portion 22 of the magnetostrictive rod 2.
Further, a pair of female screw portions 553 are formed in the
vicinities of both end portions of the first level surface 551 of
the multi-level portion 55 in a width direction thereof so as to
pass through the multi-level portion 55 in a thickness direction
thereof. The pair of female screw portions 553 are configured to be
screwed with two male screws 53, respectively.
A constituent material for each of the first block bodies 4 and the
second block bodies 5 is not particularly limited to a specific
kind as long as it has an enough stiffness for reliably fixing the
end portions 21, 22 of the magnetostrictive rods 2 to each block
body 4, 5 and generating uniform stress in the magnetostrictive
rods 2 and enough ferromagnetism for applying a bias magnetic field
generated from two permanent magnets 6 to the magnetostrictive rods
2. Examples of the constituent material having the above properties
include a pure iron (e.g., "JIS SUY"), a soft iron, a carbon steel,
a magnetic steel (silicon steel), a high-speed tool steel, a
structural steel (e.g., "JIS SS400"), a stainless, a permalloy and
a combination of two or more of these materials.
A width of each of the first block bodies 4 and the second block
bodies 5 is designed so as to be larger than a width of the
magnetostrictive rod 2. Specifically, each of the first block
bodies 4 and the second block bodies 5 has a width which enables
the magnetostrictive rods 2 to be arranged between the pairs of
female screw portions 412, 553 when the base end portions 21 of the
magnetostrictive rods 2 are inserted into the slits 411 of the
first block bodies 4 and the tip end portions 22 of the
magnetostrictive rods 2 are placed on the first level surfaces 551
of the second block bodies 5. The width of each block body 4, 5 as
described above is preferably in the range of about 3 to 15 mm, and
more preferably in the range of about 5 to 10 mm. By setting the
width of each block body 4, 5 to fall within the above range, it is
possible to downsize the power generator 1 and sufficiently ensure
a size of each of the coils 3 respectively wound around the
magnetostrictive rods 2.
The two permanent magnets 6 for applying the bias magnetic field to
the magnetostrictive rods 2 are respectively provided between the
first block bodies 4 and between the second block bodies 5.
(Permanent Magnet 6)
Each of the permanent magnets 6 has a columnar shape.
As shown in FIG. 4, the permanent magnet 6 provided between the
first block bodies 4 is arranged so that its south pole is directed
toward the lower side in FIG. 4 and its north pole is directed
toward the upper side in FIG. 4. Further, the permanent magnet 6
provided between the second block bodies 5 is arranged so that its
south pole is directed toward the upper side in FIG. 4 and its
north pole is directed toward the lower side in FIG. 4. Namely,
each of the permanent magnets 6 is arranged so that a magnetization
direction of each of the permanent magnets 6 coincides with an
arrangement direction of the magnetostrictive rods 2 (see FIG. 5).
With this configuration, a magnetic field loop circulating in the
clockwise direction is formed in the power generator 1.
As the permanent magnet 6, it is possible to use an alnico magnet,
a ferrite magnet, a neodymium magnet, a samarium-cobalt magnet, a
magnet (a bonded magnet) obtained by molding a composite material
prepared by pulverizing and mixing at least one of these magnets
with a resin material or a rubber material, or the like. In order
to more fixedly attach the permanent magnets 6 to each block body
4, 5, it is preferable to use a method for bonding the permanent
magnets 6 to each block body 4, 5 with an adhesive agent or the
like.
In the power generator 1, the permanent magnet 6 provided between
the second block bodies 5 is configured to be displaced together
with the second block bodies 5. Thus, friction does not occur
between the second block bodies 5 and the permanent magnet 6. Since
energy for displacing the second block bodies 5 is not consumed by
this friction in the power generator 1, the power generator 1 can
efficiently generate the electric power.
The magnetostrictive rods 2 as described above are connected with
each other by a connecting portion 7 through the first block bodies
4 and the second block bodies 5.
(Connecting Portion 7)
The connecting portion 7 includes a first connecting member 71 for
connecting the first block bodies 4 with each other, a second
connecting member 72 for connecting the second block bodies 5 with
each other and one beam member 73 for connecting the first
connecting member 71 and the second connecting member 72.
In this embodiment, each of the first connecting member 71, the
second connecting member 72 and the beam member 73 has a belt-like
shape (elongated plate-like shape). The connecting portion 7 has an
H-like shape in a planar view as a whole. Although the connecting
portion 7 may take a configuration in which the members are
connected with each other with a welding method or the like, it is
preferable that the connecting portion 7 takes a configuration in
which the members are formed integrally with each other.
The first connecting member 71 is configured to make contact with
an upper surface of the tall block body 41 of each of the first
block bodies 4. The second connecting member 72 is configured so
that a part of the second connecting member 72 makes contact with
the second level surface 552 of each of the second block bodies
5.
As shown in FIGS. 3(a) and 3(b), the power generator 1 of this
embodiment is configured so that a height from the upper surface to
the lower surface of the tall block body 41 of the first block body
4 (a thickness of the first block body 4 at the tall block body 41)
is higher than a height from a lower surface to an upper surface of
the second level surface 552 of the second block body 5 (a
thickness of the second block body 5 at the second level surface
552) in a side view. Thus, the power generator 1 of this embodiment
is configured so that a separation distance between the
magnetostrictive rod 2 and the first connecting member 71 is longer
than a separation distance between the magnetostrictive rod 2 and
the second connecting member 72. With this configuration, a gap
between the magnetostrictive rod 2 and the beam member 73
connecting the first connecting member 71 and the second connecting
member 72 decreases from the base end side toward the tip end side
in the side view.
For example, the connecting portion 7 having such a configuration
can be obtained by preparing a plate material having an H-shaped in
a planar view thereof and then bending the plate material with a
press work, a bending work, a hammering work or the like so that
the first connecting member 71 and the second connecting member 72
are bent from the beam member 73 respectively in two directions
opposite to each other. By using such a method for obtaining the
connecting portion 7, it is possible to easily and arbitrarily
adjust an angle formed by the first connecting member 71 and the
beam member 73 and an angle formed by the second connecting member
72 and the beam member 73.
The first connecting member 71 includes four through-holes 711
formed at four positions respectively corresponding to the four
female screw portions 412 formed in the two first block bodies 4.
The base end portions 21 of the magnetostrictive rods 2 are
inserted into the slits 411 and the male screws 43 are screwed with
the female screw portions 412 passing through the through-holes 711
of the first connecting member 71. With this configuration, the
base end portions 21 (the magnetostrictive rods 2) are fixed to the
first block bodies 4 when the first connecting member 71 is
screw-fixed to each of the tall block bodies 41 (the first block
bodies 4) to narrow spaces in the slits 411.
The second connecting member 72 includes four through-holes 721
formed at four positions respectively corresponding to the four
female screw portions 553 formed in the two second block bodies 5.
The male screws 53 are screwed with the female screw portions 553
passing through the through-holes 711 in a state that the tip end
portions 22 of the magnetostrictive rods 2 are placed on the first
level surfaces 551 of the second block bodies 5 and a base end
portion of the second connecting member 72 makes contact with the
second level surfaces 552 of the second block bodies 5. With this
configuration, the second connecting member 72 is screw-fixed to
the second block bodies 5 and the tip end portions 22 are gripped
between a lower surface of the second connecting member 72 and the
first level surfaces 551 of the second block bodies 5. Thus, the
tip end portions 22 (the magnetostrictive rods 2) are fixed to the
second block bodies 5.
As described above, the magnetostrictive rods 2 and the first
connecting member 71 are fastened to the first block bodies 4 with
the male screws 43, and the magnetostrictive rods 2 and the second
connecting member 72 are fastened to the second block bodies 5 with
the male screws 53. Thus, it is possible to reduce the number of
parts and the number of steps for fixing and connecting the members
with each other. In this regard, a fixing and connecting method is
not limited to the above screwing method. Examples of the fixing
and connecting method include a caulking method, a diffusion
bonding method, a pin pressure fitting method, a brazing method, a
welding method (such as a laser welding method and an electric
welding method) and a bonding method with an adhesive agent.
By adjusting lengths of the first connecting member 71 and the
second connecting member 72, it is possible to change the gap
between the magnetostrictive rods 2. By enlarging the gap between
the magnetostrictive rods 2, it is possible to sufficiently ensure
spaces for respectively winding the coils 3 around the
magnetostrictive rods 2. With this configuration, it is possible to
sufficiently enlarge the sizes of the coils 3, thereby improving
the power generation efficiency of the power generator 1.
The beam member 73 connects a central portion of the first
connecting member 71 and a central portion of the second connecting
member 72. In the power generator 1, this beam member 73 and the
magnetostrictive rods 2 are arranged so as not to overlap with each
other in the planar view (see FIG. 1) and configured so that the
gap between the beam member 73 and the magnetostrictive rods 2
decreases from the base end side to the tip end side in the side
view (see FIG. 3). In this embodiment, a width of the beam member
73 is set so as to be smaller than a gap between the coils 3
respectively wound around the magnetostrictive rods 2. Further, the
beam member 73 is configured to overlap with the coils 3 on the tip
end side in the side view.
In the power generator 1, the magnetostrictive rods 2 and the beam
member 73 serve as beams facing each other. The magnetostrictive
rods 2 and the beam member 73 are displaced in the same direction
(the upper direction or the lower direction in FIG. 1) together
when the second block bodies 5 are displaced. At this time, stress
is generated in each of the magnetostrictive rods 2 due to the beam
member 73. At this time, since the beam member 73 is arranged
between the coils 3 respectively wound around the magnetostrictive
rods 2, each of the magnetostrictive rods 2 does not make contact
with the beam member 73 when each of the magnetostrictive rods 2 is
displaced.
Further, the connecting portion 7 is configured so that a length of
the beam member 73 before the connecting portion 7 is connected to
the first block bodies 4 and the second block bodies 5 is longer
than a length from tip end portions of the first block bodies 4 to
base end portions of the second block bodies 5 connected to the
magnetostrictive rods 2 in the planar view. In this embodiment, the
first block bodies 4 and the second block bodies 5 are connected
with each other by the connecting portion 7 having the beam member
73 as described above. Thus, in the power generator 1, the second
block bodies 5 are pressed toward the lower direction (the right
and lower direction in FIG. 3(b)) by the beam member 73 to displace
the second block bodies 5 with respect to the first block bodies 4.
With this configuration, the base end portions 21 and the tip end
portions 22 of the magnetostrictive rods 2 approach to each other
in a natural state (that is a state that external force is not
applied to the power generator 1) (see FIG. 3(b)). As a result,
compressive stress is generated in each of the magnetostrictive
rods 2. In this embodiment, the beam member 73 described above
constitutes a bias stress generating mechanism for generating bias
stress (the compressive stress) in the magnetostrictive rods 2 in
the natural state.
The power generator 1 as described above is used in a state that
the first block bodies 4 are fixed to a housing 100 of the
vibrating body through the male screws 44 (see FIG. 6(a)). In this
state, when the second block bodies 5 are displaced (pivotally
moved) with respect to the first block bodies 4 in the lower
direction by the vibration of the vibrating body (see FIG. 6(b)),
that is when the tip end portions 22 of the magnetostrictive rods 2
are displaced with respect to the base end portions 21 of the
magnetostrictive rods 2 in the lower direction, the beam member 73
is deformed so as to be expanded in an axial direction thereof and
the magnetostrictive rods 2 are deformed so as to be contracted in
the axial direction thereof. On the other hand, when the second
block bodies 5 are displaced (pivotally moved) in the upper
direction, that is when the tip end portions 22 of the
magnetostrictive rods 2 are displaced with respect to the base end
portions 21 of the magnetostrictive rods 2 in the upper direction,
the beam member 73 is deformed so as to be contracted in the axial
direction thereof and the magnetostrictive rods 2 are deformed so
as to be expanded in the axial direction thereof. As a result, the
magnetic permeability of each of the magnetostrictive rods 2 varies
due to the inverse magnetostrictive effect. This variation of the
magnetic permeability of each of the magnetostrictive rods 2 leads
to the variation of the density of the lines of magnetic force
passing through the magnetostrictive rods 2 (the density of the
lines of magnetic force passing through the coils 3), thereby
generating the voltage in the coils 3.
In the power generator 1 described above, a magnitude of the
voltage (a power generation amount) generated in the coils 3 is
proportional to the variation amount of the magnetic flux density
of each of the magnetostrictive rods 2. The variation amount of the
magnetic flux density of each of the magnetostrictive rods 2
depends on an intensity of the applied bias magnetic field and a
magnitude of the stress (the tensile stress or the compressive
stress) generated in each of the magnetostrictive rods 2.
FIG. 7 is graphs showing a relationship between magnetic flux
density (B) and a bias magnetic field (H) applied to the
magnetostrictive rod formed of the magnetostrictive material
containing the iron-gallium based alloy (having the Young's modulus
of about 70 GPa) as the main component thereof depending on the
stress generated in the magnetostrictive rod and a relationship
between a variation amount of the magnetic flux density (.DELTA.B)
and the applied bias magnetic field (H), as concrete examples.
Specifically, each of FIGS. 7(a) and 7(b) is a graph showing the
relationship between the magnetic flux density (B) and the bias
magnetic field (H) applied to the magnetostrictive rod depending on
the stress generated in the magnetostrictive rod. FIG. 7(c) is a
graph showing the relationship between the variation amount of the
magnetic flux density (.DELTA.B) and the bias magnetic field (H)
applied to the magnetostrictive rod depending on the stress
generated in the magnetostrictive rod. In this graph, a state in
that the stress does not occur in the magnetostrictive rod is
utilized as a reference. FIG. 7(d) is a graph showing the
relationship between the variation amount of the magnetic flux
density (.DELTA.B) and the bias magnetic field (H) applied to the
magnetostrictive rod depending on the stress generated in the
magnetostrictive rod. In this graph, a state that compressive
stress of 14.15 MPa occurs in the magnetostrictive rod is utilized
as a reference.
In this regard, the relationship (H-B curve) between the magnetic
flux density (B) and the bias magnetic field (H) in a state that
the stress (.+-.0 MPa) does not occur in the magnetostrictive rod
is represented by a heavy line in FIG. 7(a). Further, the
relationship (H-B curve) between the magnetic flux density (B) and
the bias magnetic field (H) in a state that the compressive stress
of 14.15 MPa (-14.15 MPa) occurs in the magnetostrictive rod is
represented by a heavy line in FIG. 7(b). In the following
description, for example, the language of "the stress of .+-.14.15
MPa is generated" in the magnetostrictive rod in which the bias
stress is not generated in the natural state means a situation that
the tensile stress of 14.15 MPa (+14.15 MPa) and the compressive
stress of 14.15 MPa (-14.15 MPa) are alternately generated in the
magnetostrictive rod.
As shown in FIG. 7(a), the magnetic permeability of the
magnetostrictive rod in which the tensile stress occurs is higher
than the magnetic permeability of the magnetostrictive rod in which
the stress does not occur. In addition, this tendency becomes
remarkable as the tensile stress generated in the magnetostrictive
rod increases. As a result, the density of the lines of magnetic
force (the magnetic flux density) passing through the
magnetostrictive rod in the axial direction thereof becomes higher
as the tensile stress generated in the magnetostrictive rod
increases (see H-B curves positioned on the upper side of the heavy
line in FIG. 7(a)). On the other hand, the magnetic permeability of
the magnetostrictive rod in which the compressive stress occurs is
lower than the magnetic permeability of the magnetostrictive rod in
which the stress does not occur. This tendency becomes remarkable
as the compressive stress generated in the magnetostrictive rod
increases. As a result, the density of the lines of magnetic force
(the magnetic flux density) passing through the magnetostrictive
rod in the axial direction thereof becomes lower as the compressive
stress generated in the magnetostrictive rod increases (see H-B
curves positioned on the lower side of the heavy line in FIG.
7(a)).
As shown in FIG. 7(a), in the magnetostrictive rod as described
above, the variation amount of the magnetic flux density (magnetic
permeability) caused by the generation of the compressive stress is
large. Namely, the decreasing amount of the magnetic flux density
of the magnetostrictive rod from a state that the stress does not
occur in the magnetostrictive rod is large. On the other hand, the
variation amount of the magnetic flux density (magnetic
permeability) caused by the generation of the tensile stress is
small. Namely, the increasing amount of the magnetic flux density
of the magnetostrictive rod from a state that the stress does not
occur in the magnetostrictive rod is small.
Thus, even if the tensile stress and the compressive stress having
a certain magnitude are alternately generated in the
magnetostrictive rod in which the bias stress is not generated in
the natural state, the variation amount of the magnetic flux
density caused by this tensile stress is small. Therefore,
depending on the intensity of the applied bias magnetic field, it
is difficult to sufficiently vary the magnetic flux density of the
magnetostrictive rod.
For example, as shown in FIG. 7(c), when the stress of .+-.14.15
MPa is generated in the magnetostrictive rod in which the bias
stress is not generated in the natural state, the intensity of the
bias magnetic field required for obtaining the variation amount of
the magnetic flux density (.DELTA.B) equal to or more than 1 T is
about 0.8 to 2.8 kA/m. Further, when the stress of .+-.49.56 MPa is
generated in such a magnetostrictive rod, the intensity of the bias
magnetic field required for obtaining the variation amount of
magnetic flux density (.DELTA.B) equal to or more than 1 T is about
0.8 to 9.8 kA/m.
In contrast, in the power generator 1, since the compressive stress
is generated in each of the magnetostrictive rods 2 in the natural
state, the magnetic permeability of each of the magnetostrictive
rods 2 in the natural state is lower than the magnetic permeability
of the magnetostrictive rod in which the stress does not occur.
Each of the magnetostrictive rods 2 is expanded and contracted from
a basic state that the compressive stress is generated in each of
the magnetostrictive rods 2.
For example, as shown in FIG. 7(b), when the compressive stress of
14.15 MPa is generated in each of the magnetostrictive rods 2 in
the natural state, each of the magnetostrictive rods 2 is expanded
and contracted from a basic state represented by the heavy line in
FIG. 7(b). In this case, the variation amount (increasing amount)
of the magnetic flux density caused by the generation of the
tensile stress is larger than the variation amount of the magnetic
flux density when the tensile stress is generated in the
magnetostrictive rod in which the bias stress is not generated in
the natural state.
Thus, in the magnetostrictive rods 2 of the power generator 1, it
is possible to increase the variation amount of the magnetic flux
density caused by the generation of the compressive stress and the
variation amount of the magnetic flux density caused by the
generation of the tensile stress. With this configuration, it is
possible to broaden a range of intensities of the bias magnetic
field required for obtaining the sufficient variation amount of the
magnetic flux density (equal to or more than 1 T).
For example, as shown in FIG. 7(d), the stress of .+-.14.15 MPa is
generated in the magnetostrictive rod in which the compressive
stress of 14.15 MPa is generated in the natural state. Namely, the
tensile stress and the compressive stress alternately generated in
the magnetostrictive rod are set to be respectively 0 MPa and -28.3
MPa. At this time, the intensity of the bias magnetic field
required for obtaining the variation amount of the magnetic flux
density (.DELTA.B) equal to or more than 1 T is about 1.6 to 5.7
kA/m. Further, the stress of .+-.49.56 MPa is generated in such a
magnetostrictive rod. Namely, the tensile stress and the
compressive stress alternately generated in the magnetostrictive
rod are set to be respectively +35.4 MPa and -63.71 MPa. At this
time, the intensity of the bias magnetic field required for
obtaining the variation amount of the magnetic flux density
(.DELTA.B) equal to or more than 1 T is about 0.7 to 13 kA/m.
The comparison of FIGS. 7(c) and 7(d) indicates that the range of
intensities of the bias magnetic field required for obtaining the
sufficient variation amount of the magnetic flux density can be
broadened by generating the compressive stress (the bias stress) in
the magnetostrictive rod in the natural state.
As described above, in the power generator 1, the range of
intensities of the bias magnetic field required for generating the
sufficient variation amount of the magnetic flux density in each of
the magnetostrictive rods 2 is broadened. Thus, for example, it is
possible to generate the variation of the magnetic flux density in
each of the magnetostrictive rods 2 in the same manner even if a
different magnet having a different size or a different shape is
used as the permanent magnet 6 or a different magnet having
different characteristics such as attracting force or a maximum
energy product is used as the permanent magnet 6. Further, even if
the positional relationship between the magnetostrictive rods 2 and
the permanent magnets 6 is changed and the intensity of the bias
magnetic field applied to the magnetostrictive rods 2 is changed,
it is possible to generate the sufficient variation of the magnetic
flux density in each of the magnetostrictive rods 2. As described
above, in the power generator 1, it is possible to sufficiently
increase the variation amount of the magnetic flux density of each
of the magnetostrictive rods 2 even if the configuration (the size,
the position or the like of each component) of the power generator
1 is changed with a certain level of freedom for design. Namely, it
is possible to increase a degree of freedom for designing the power
generator 1. Further, the power generator 1 can obtain a large
power generation amount in a wide range of intensities of the bias
magnetic field. Thus, even if variation in the intensity of the
bias magnetic field applied to the magnetostrictive rods 2 is
caused by an assembly error generated by errors of material
characteristics of the components constituting the power generator
1, shape tolerance of the components, positional shifts of
attachment positions of the components at the time of assembling
the power generator 1 or the like, the power generator 1 can stably
obtain the sufficient large power generation amount.
Further, in the power generator 1, each of the magnetostrictive
rods 2 is expanded and contracted from the basic state that the
compressive stress is generated in each of the magnetostrictive
rods 2. When the same external force is applied to the
magnetostrictive rods 2 and the magnetostrictive rod in which the
stress is not generated in the natural state, the magnitude of the
compressive stress generated in each of the magnetostrictive rods 2
is smaller than the magnitude of the compressive stress generated
in the magnetostrictive rod (which is expanded and contracted from
a basic state that the stress is not generated in the
magnetostrictive rod in the natural state). Generally, when the
tensile stress is repeatedly generated in one member, the member is
likely to be deteriorated and its durability also deteriorates. On
the other hand, since the compressive stress is generated in each
of the magnetostrictive rods 2 of the power generator 1 in the
natural state, it is possible to prevent the magnetostrictive rods
2 from being deteriorated and keep their superior durability even
if the power generator 1 is repeatedly used.
In particular, selectable kinds of the described constituent
material for the magnetostrictive rods 2 are limited and the
constituent material for the magnetostrictive rods 2 has relatively
low stiffness. In the power generator 1, by using a material having
relatively high stiffness as described below as the constituent
material for the beam member 73 serving as the parallel beams in
cooperation with the magnetostrictive rods 2, it is possible to
improve durability of the magnetostrictive rods 2 and the beam
member 73 (connecting portion 7) and extend a product lifetime of
the power generator 1.
Further, as described above, the power generator 1 is configured so
that the gap between the magnetostrictive rods 2 and the beam
member 73 (hereinafter, this gap is referred to as "beam gap")
decreases from the base end side to the tip end side in the side
view. In other words, the magnetostrictive rods 2 and the beam
member 73 form a beam structure (tapered beam structure) tapering
from the base end side to the tip end side (see FIG. 3(b)). In such
a structure, stiffness of a pair of beams constituted of the
magnetostrictive rods 2 and the beam member 73 in a displacement
direction (the vertical direction) thereof decreases from the base
end side to the tip end side. Thus, when the external force is
applied to the tip end portion of the power generator 1 (the second
block bodies 5), the magnetostrictive rods 2 and the beam member 73
can be smoothly displaced in the vertical direction. As a result,
it is possible to reduce variation in the stress generated in each
of the magnetostrictive rods 2 in the thickness direction thereof,
thereby generating uniform stress in each of the magnetostrictive
rods 2.
As described above, according to the power generator 1, it is
possible to sufficiently increase the variation amount of the
magnetic flux density of each of the magnetostrictive rods 2 in the
wide range of intensities of the bias magnetic field even if the
tensile stress and the compressive stress generated in each of the
magnetostrictive rods 2 are relatively small. In addition, since it
is possible to reduce the variation in the stress generated in each
of the magnetostrictive rods 2 and generate the uniform stress in
each of the magnetostrictive rods 2, the power generator 1 can
efficiently generate the electric power by utilizing the applied
external force.
Further, according to the power generator 1, it is possible to
freely design the beam gap between the magnetostrictive rods 2 and
the beam member 73. Specifically, by adjusting a length (height)
from the slit 411 formed on each of the first block bodies 4 to the
upper surface of each of the first block bodies 4 (the upper
surface of the tall block body 41), it is possible to freely design
the beam gap between the magnetostrictive rods 2 and the beam
member 73 on the base end side. Thus, it is possible to freely
design the beam gap between the magnetostrictive rods 2 and the
beam member 73.
A relationship between the beam gap between the pair of beams and
the stress generated when the external force is applied to tip end
portions of the pair of beams has been analyzed by the inventors of
the present invention. Further, from the following results of
study, it has been found that substantially uniform stress is
generated in each beam when the beam gap decreases.
FIG. 8 is a side view schematically showing a state that external
force in the lower direction is applied to a tip end portion of one
rod member (one beam) whose base end portion is fixed to a housing.
FIG. 9 is a side view schematically showing a state that external
force in the lower direction is applied to the tip end portions of
the pair of beams (parallel beams) parallel arranged so as to face
each other whose base end portions are fixed to the housing. FIG.
10 is a view schematically showing the stress (the tensile stress
and the compressive stress) generated in the pair of parallel beams
when the external force is applied to the tip end portions of the
pair of parallel beams.
Hereinafter, an upper side in each of FIGS. 8 to 10 is referred to
as "upper" or "upper side" and a lower side in each of FIGS. 8 to
10 is referred to as "lower" or "lower side". Further, a left side
in each of FIGS. 8 to 10 is referred to as "base end side" and a
right side in each of FIGS. 8 to 10 is referred to as "tip end
side".
When the external force is applied to the tip end portion of one
beam so that the beam is bent and deformed in the lower direction
as shown in FIG. 8, the stress is generated in the beam due to this
bending deformation of the beam. At this time, uniform tensile
stress (stretching stress) is generated on an upper portion of the
beam and uniform compressive stress (contraction stress) is
generated on a lower portion of the beam. On the other hand, when
the external force is applied to the tip end portions of the
parallel beams having a certain beam gap, the pair of beams are
deformed with two states simultaneously occurring. One of the two
states is that each beam is bent and deformed as shown in FIG. 8.
The other one of the two states is that the pair of beams are
deformed as shown in FIG. 9 so as to perform a parallel link
movement for keeping the beam gap on the tip end side constant
before and after the external force is applied. In the parallel
beams, this parallel link operation becomes marked as the beam gap
increases. On the other hand, the parallel link operation is
suppressed as the beam gap decreases. Thus, the deformations of the
parallel beams become similar to the bending deformation of the one
beam as shown in FIG. 8 as the beam gap decreases.
Thus, the bending deformation as shown in FIG. 8 and the
deformations due to the parallel link movement as shown in FIG. 9
simultaneously occur in the configuration of the parallel beams
having a relatively large beam gap. As a result, each beam is
deformed in a substantially S-like shape as shown in FIG. 10. When
the parallel beams are deformed in the lower direction, it is
preferable that uniform tensile stress is generated in the upper
beam. Actually, as shown in FIG. 10, although tensile stress A is
generated in a central portion of the upper beam, large compressive
stress B is generated in a lower portion of the upper beam on the
base end side and an upper portion of the upper beam on the tip end
side. Further, it is preferable that uniform compressive stress is
generated in the lower beam. Actually, although the compressive
stress B is generated in a central portion of the lower beam, the
large tensile stress A is generated in an upper portion of the
lower beam on the base end side and a lower portion of the lower
beam on the tip end side. Namely, since both of the tensile stress
A and the compressive stress B generated in each beam are large, it
is impossible to increase an absolute value of one of the tensile
stress and the compressive stress generated in an entire of the
beam. Thus, in the case of using the described parallel beams as
the magnetostrictive rods, it is impossible to increase the
variation amount of the magnetic flux density in each of the
magnetostrictive rods.
From the above results of study, the following fact has been found.
Namely, from a point of view of improving the power generation
efficiency, it is preferable that the power generator whose
magnetostrictive rods and beam member constitute the pair of
parallel beams are configured so that a behavior of a bending
deformation of the pair of parallel beams becomes similar to a
behavior of the bending deformation of one beam as shown in FIG. 8
by decreasing the beam gap between the magnetostrictive rods and
the beam member to suppress the parallel link movement of the
beams.
Further, in the power generator 1, since the size of each of the
coils 3 is not limited by the beam gap between the magnetostrictive
rods 2 and the beam member 73, it is possible to sufficiently
increase the size of each of the coils 3 and design the power
generator 1 so that the beam gap between the magnetostrictive rods
2 and the beam member 73 becomes sufficiently small. With this
configuration, it is possible to increase the size of each of the
coils 3 and more uniform the stress generated in each of the
magnetostrictive rods 2, thereby improving the power generation
efficiency of the power generator 1.
Further, in the power generator 1, the stiffness of the pair of
beams constituted of the magnetostrictive rods 2 and the beam
member 73 in the displacement direction decreases from the base end
side to the tip end side. Thus, it is possible to drastically
deform the magnetostrictive rods 2 in the vertical direction with
relatively small external force.
In this regard, although a value of the magnitude of the
compressive stress generated in each of the magnetostrictive rods 2
in the natural state by the beam member 73 is particularly not
limited to a specific value, the range of intensities of the bias
magnetic field required for sufficiently ensuring the variation
amount of the magnetic flux density generated in each of the
magnetostrictive rods 2 is broadened (widened) as the generated
compressive stress increases. For example, in the case of using the
magnetostrictive material containing the iron-gallium based alloy
(having the Young's modulus of about 70 GPa) as the main component
thereof as the constituent material for the magnetostrictive rods
2, the compressive stress generated in each of the magnetostrictive
rods 2 in the natural state is preferably in the range of about 5
to 50 MPa, and more preferably in the range of about 10 to 40
MPa.
In this regard, an angle formed by the beam member 73 and each of
the magnetostrictive rods 2 (taper angle) in the side view is not
particularly limited to a specific value, but is preferably in the
range of about 0.5 to 7.degree., and more preferably in the range
of about 1 to 4.degree.. If the angle formed by the beam member 73
and each of the magnetostrictive rods 2 is in the above range, it
is possible to form the above tapered beam structure with the
magnetostrictive rods 2 and the beam member 73 and sufficiently
decrease the beam gap between the magnetostrictive rods 2 and the
beam member 73 on the base end side. With this configuration, it is
possible to generate more uniform stress in each of the
magnetostrictive rods 2.
As a constituent material for the connecting portion 7 as described
above, it is preferable to use a material which can prevent the
magnetic field loop formed by the magnetostrictive rods 2 and the
permanent magnets 6 from short-circuiting due to the connecting
portion 7 (beam member 73). Thus, although it is preferable that
the connecting portion 7 is formed of a weakly magnetic material or
a non-magnetic material, it is more preferable from a point of view
of more reliably preventing the short-circuit of the magnetic field
loop that the connecting portion 7 is formed of the non-magnetic
material.
Although a spring constant of the beam member 73 as described above
may be different from a spring constant of each of the
magnetostrictive rods 2, it is preferable that the spring constant
of the beam member 73 is equal to a total value of the spring
constants of all of the magnetostrictive rods 2, that is a total
value of the spring constants of the two magnetostrictive rods 2.
As described above, in this embodiment, the two magnetostrictive
rods 2 and the one beam member 73 serve as the pair of beams facing
each other. Thus, by using the beam member 73 (connecting portion
7) satisfying the above condition, it is possible to uniform the
stiffness in the vertical direction between the beam member 73 and
the magnetostrictive rods 2. With this configuration, it is
possible to smoothly and reliably displace the second block bodies
5 with respect the first block bodies 4 in the vertical
direction.
Further, generally, when external force F is applied to a movable
end portion (other end portion) of a cantilevered beam whose one
end portion is fixed, a deformation (bending amount) d of the beam
can be expressed by the following formula (2). d=FL.sup.3/3EI
(2)
(wherein "L" is a length of the beam, "E" is a Young's modulus of a
constituent material for the beam and "I" is a cross-sectional
secondary moment of the beam)
In the power generator 1, cross-sectional areas of each
magnetostrictive rod 2 and the beam member 73 are substantially
equal to each other as shown in FIG. 3(b). Thus, cross-sectional
secondary moments of each magnetostrictive rod 2 and the beam
member 73 are also substantially equal to each other. Further,
lengths of each magnetostrictive rod 2 and the beam member 73 are
substantially equal to each other. Thus, according to the above
formula (2), in the case where the power generator 1 takes a
configuration in which the number of the beam members 73 is one and
the number of the magnetostrictive rods 2 is two, it is preferable
that a Young's modulus of the beam member 73 is set to be about
twice of a Young's modulus of each magnetostrictive rod 2. With
this configuration, each beam (each of the beam member 73 and the
two magnetostrictive rods 2) is similarly deformed (bent) by the
external force. In other words, it is possible to achieve a good
balance among the stiffness of each beam in the vertical
direction.
Further, the Young's modulus of the beam member 73 as described
above is preferably in the range of about 80 to 200 GPa, more
preferably in the range of about 100 to 190 GPa, and even more
preferably in the range of about 120 to 180 GPa.
The non-magnetic material having the above Young's modulus is not
particularly limited to a specific kind. Examples of such a
non-magnetic material include a metallic material, a semiconductor
material, a ceramic material, a resin material and a combination of
two or more of these materials. In the case of using the resin
material as the non-magnetic material, it is preferred that filler
is added into the resin material. Among them, a non-magnetic
material containing a metallic material as a main component thereof
is preferably used. Further, a non-magnetic material containing at
least one selected from the group consisting of stainless steel,
beryllium copper, aluminum, magnesium, zinc, copper and an alloy
containing at least one of these materials as a main component
thereof is more preferably used.
In the case of using the magnetostrictive material containing the
iron-gallium based alloy (having the Young's modulus of about 70
GPa) as the main component thereof as the constituent material for
the magnetostrictive rods 2, it is preferable to use the stainless
steel ("SUS 316", having a Young's modulus of about 170 GPa) as the
constituent material for the connecting portion 7. By using these
materials respectively having these above Young's modulus as the
constituent materials for the magnetostrictive rods 2 and the beam
member 73, it is possible to achieve a good balance among the
stiffness of the beam member 73 and the two magnetostrictive rods 2
in the vertical direction. With this configuration, it is possible
to smoothly and reliably displace the second block bodies 5 with
respect to the first block bodies 4 in the vertical direction.
A thickness (cross-sectional area) of the beam member 73 as
described above is substantially constant. An average thickness of
the beam member 73 is not particularly limited to a specific value,
but is preferably in the range of about 0.3 to 10 mm, and more
preferably in the range of about 0.5 to 5 mm. Further, an average
cross-sectional area of the beam member 73 is preferably in the
range of about 0.2 to 200 mm.sup.2, and more preferably in the
range of about 0.5 to 50 mm.sup.2.
The air-conditioning duct to which the power generator 1 is fixedly
attached is, for example, a duct or a pipe used for forming a flow
channel in a device for delivering (discharging, ventilating,
inspiring, wasting or circulating) steam, water, fuel oil and gas
(such as air and fuel gas). Examples of the pipe and the duct
include an air-conditioning duct installed in a big facility,
building, station and the like. Further, the vibrating body to
which the power generator 1 is attached is not limited to such an
air-conditioning duct. Examples of the vibrating body include a
transportation (such as a freight train, an automobile and a back
of truck), a crosstie (skid) for railroad, a wall panel of an
express highway or a tunnel, a bridge, a vibrating device such as a
pump and a turbine.
The vibration of the vibrating body is unwanted vibration for
delivering an objective medium (in the case of the air-conditioning
duct, gas and the like passing through the duct). The vibration of
the vibrating body normally results in noise and uncomfortable
vibration. In the present invention, by fixedly attaching the power
generator 1 to such a vibrating body, it is possible to generate
electric energy in the power generator 1 by converting
(regenerating) such unwanted vibration (kinetic energy).
The power generator 1 can be utilized for a power supply of a
sensor, a wireless communication device and the like. For example,
the power generator 1 can be utilized in a system containing a
sensor and a wireless communication device. In this system, by
utilizing the electric energy (electric power) generated by the
power generator 1 to drive the sensor, the sensor can get measured
data such as illumination intensity, temperature, humidity,
pressure and noise in a facility or a residential space. Further,
by utilizing the electric power generated by the power generator 1
to drive the wireless communication device, the wireless
communication device can transmit the data measured by the sensor
to an external device (such as a server and a host computer) as
detected data. The external device can use the measured data as
various control signals or a monitoring signal. Furthermore, the
power generator 1 can be used for a system for monitoring status of
each component of vehicle (for example, a tire pressure sensor and
a sensor for seat belt wearing detection). Further, by converting
such unwanted vibration of the vibrating body to the electric
energy with the power generator 1, it is possible to provide an
effect of reducing the noise and the uncomfortable vibration
generated from the vibrating body.
Further, in addition to the intended use of regenerating the
vibration from the vibrating body as described above, by providing
the power generator 1 with a mechanism for directly applying the
external force to the tip end portion of the power generator 1 (the
second block bodies 5) and combining the power generator 1 with a
wireless communication device, it is possible to obtain a switching
device which can be manually operated by a user. Such a switching
device can function without being wired for a power supply
(external power supply) and a signal line. For example, the
switching device can be used for a wireless switch for house
lighting, a home security system (in particular, a system for
wirelessly informing detection of operation of a window or a door)
or the like.
Further, by applying the power generator 1 to each switch of a
vehicle, it becomes unnecessary to wire the switch for the power
supply and the signal line. With such a configuration, it is
possible to reduce the number of assembling steps and a weight of a
wire provided in the vehicle, thereby achieving weight saving of
the vehicle or the like. This makes it possible to suppress a load
on a tire, a vehicle body and an engine and contribute to safety of
the vehicle.
Although the coils 3 respectively wound around the magnetostrictive
rods 2 and the beam member 73 are arranged so as not to overlap
with each other in the planar view in the power generator 1
according to this embodiment, it may be possible to take a
configuration in which parts of the coils 3 overlap with the beam
member 73. Specifically, it may be possible to take a configuration
in which the magnetostrictive rods 2 and the beam member 73 do not
overlap with each other in the planar view and end portions of the
coils 3 and the end portions of the beam member 73 overlap with
each other in the planar view. Even in the case of taking such a
configuration, it is possible to sufficiently ensure the winding
spaces for the coils 3 and sufficiently decrease the beam gap
between the magnetostrictive rods 2 and the beam member 73 within a
range that the coils 3 and the beam member 73 do not make contact
with each other, thereby providing the same effect as the effect
provided by the above power generator 1.
The power generation amount of the power generator 1 is not
particularly limited to a specific value, but is preferably in the
range of about 20 to 2000 .mu.J. If the power generation amount of
the power generator 1 (power generating capability of the power
generator 1) is in the above range, it is possible to efficiently
utilize the electric power generated by the power generator 1 for
the wireless switch for house lighting, the home security system or
the like described above in combination with a wireless
communication device.
Although the power generator 1 of this embodiment includes the two
magnetostrictive rods 2 and the one beam member 73 as the beams
facing each other, the present invention is not limited thereto.
The present invention may take a configuration as described
below.
FIG. 11 is a planar view showing another configuration example of
the power generator of the first embodiment of the present
invention.
In the power generator 1 shown in FIG. 11, the connecting portion 7
includes two beam members 73 for respectively connecting the end
portions of the first connecting member 71 in the longitudinal
direction thereof and the end portions of the second connecting
member 72 in the longitudinal direction thereof. In this
configuration, since the beam members 73 are arranged on the outer
side of the magnetostrictive rods 2, it is possible to increase the
size of each of the coils 3 and decrease the gap between the
magnetostrictive rods 2, thereby reducing a size of the power
generator 1 in the width direction thereof (the vertical direction
in FIG. 11). Even in the case of taking this configuration, it is
possible to provide the same effect as the effect provided by the
described embodiment.
In the above description, the connecting portion 7 is configured so
that the length of each beam member 73 is longer than the length
from the tip end portions of the first block bodies 4 to the base
end portions of the second block bodies 5 in the planar view in a
state before the connecting portion 7 is connected to each block
body 4, 5. With this configuration, when the connecting portion 7
is connected to each block body 4, 5, the beam member 73 can
generate the bias stress in each of the magnetostrictive rods 2 in
the natural state. However, the power generator 1 according to this
embodiment may take a configuration as described below.
FIG. 12(a) is a right-side view (with the coils being omitted) for
explaining the state before the connecting portion is connected to
each block body in the other configuration example of the power
generator of the first embodiment of the present invention. FIG.
12(b) is a right-side view (with the coils being omitted) of the
other configuration example of the power generator of the first
embodiment of the present invention.
Hereinafter, an upper side in each of FIGS. 12(a) and 12(b) is
referred to as "upper" or "upper side" and a lower side in each of
FIGS. 12(a) and 12(b) is referred to as "lower" or "lower side".
Further, a right side in each of FIGS. 12(a) and 12(b) is referred
to as "tip end side" and a left side in each of 12(a) and 12(b) is
referred to as "base end side".
The power generator 1 shown in FIGS. 12(a) and 12(b) is configured
so that an angle (bending angle) formed by the first connecting
member 71 and each beam member 73 and an angle (bending angle)
formed by the second connecting member 72 and each beam member 73
are larger than those of the power generator 1 shown in FIG. 3.
As shown in FIG. 12(a), in this power generator 1, a difference
between the height positions of the first connecting member 71 and
the second connecting member 72 (a height from the lower surface of
the second connecting member 72 to a lower surface of the first
connecting member 71) in the side view in a state before the
connecting portion 7 is connected to each block body 4, 5 is
"t.sub.1". The power generator 1 is configured so that a difference
t.sub.2 between the height positions of the first connecting member
71 and the second connecting member 72 in the side view in a state
that the connecting portion 7 is connected to each block body 4, 5
is smaller than the difference t.sub.1 (t.sub.1>t.sub.2) as
shown in FIG. 12(b).
By designing the connecting portion 7 so that the angles formed by
each connecting member 71, 72 and the beam member 73 become large
as described above, the second block bodies 5 are pressed toward
the lower direction in FIG. 12(b) by the beam member 73 to displace
the second block bodies 5 with respect to the first block bodies 4
in the power generator 1. With this configuration, the base end
portions 21 and the tip end portions 22 of the magnetostrictive
rods 2 approach to each other in the natural state, thereby
generating the compressive stress in each of the magnetostrictive
rods 2.
The power generator 1 having the above configuration can also
provide the same function and effect as those of the power
generator 1 of the described embodiment.
Further, the power generator 1 can take a configuration including
two or more of the magnetostrictive rods 2 and one or more of the
beam members 73. In the case of changing a total number of the
magnetostrictive rods 2 and the beam members 73, it is preferable
that this total number is an odd number. Specifically, the power
generator 1 can take a configuration in which a ratio of the number
of the magnetostrictive rods 2 and the number of the beam members
73 (the number of the magnetostrictive rods 2: the number of the
beam members 73) becomes 2:3, 3:2, 3:4, 4:3, 4:5 or the like. In
such a configuration, since the magnetostrictive rods 2 and the
beam members 73 serving as the beams are symmetrically arranged in
the width direction of the power generator 1, it is possible to
achieve a good balance among the stress generated in the
magnetostrictive rods 2, each block body 4, 5 and the connecting
portion 7.
In the case of taking the configuration as described above, when
the spring constant of each of the beam members 73 is defined as
"A" [N/m], the number of the beam members 73 is defined as "X", the
spring constant of each of the magnetostrictive rods 2 is defined
as "B" [N/m] and the number of the magnetostrictive rods 2 is
defined as "Y", it is preferable that the power generator 1 is
configured so that a value of "A.times.X" is substantially equal to
a value of "B.times.Y". With this configuration, it is possible to
smoothly and reliably displace the second block bodies 5 with
respect to the first block bodies 4 in the vertical direction.
In the above description, the connections between the both end
portions 21, 22 of the magnetostrictive rods 2 and each block body
4, 5 and the connections between the connecting portion 7 and each
block body 4, 5 are achieved by screwing the male screws 43, 53
into the female screw portions 412, 553, but the fixing and
connecting method for each component is not limited to this
screwing method. Examples of the fixing and connecting method for
each component include a caulking method, a diffusion bonding
method, a pin pressure fitting method, a brazing method, a welding
method (such as a laser welding method and an electric welding
method) and a bonding method with an adhesive agent.
Second Embodiment
Next, description will be given to a second embodiment of the power
generator of the present invention.
FIG. 13 is a side view showing the second embodiment of the power
generator of the present invention. FIG. 14 is a side view showing
another configuration example of the power generator of the second
embodiment of the present invention.
Hereinafter, an upper side in each of FIGS. 13 and 14 is referred
to as "upper" or "upper side" and a lower side in each of FIGS. 13
and 14 is referred to as "lower" or "lower side". Further, a right
side in each of FIGS. 13 and 14 is referred to as "tip end side"
and a left side in each of FIGS. 13 and 14 is referred to as "base
end side".
Hereinafter, the power generator according to the second embodiment
will be described by placing emphasis on the points differing from
the power generator according to the first embodiment, with the
same matters being omitted from the description.
The power generator 1 shown in FIG. 13 includes the
magnetostrictive rod 2 around which the coil 3 is wound, a beam
member 8 arranged along the magnetostrictive rod 2, a connecting
yoke 46 connecting the base end portion 21 of the magnetostrictive
rod 2 and a base end portion of the beam member 8, connecting yokes
56, 57 respectively provided on the tip end portion 22 of the
magnetostrictive rod 2 and a tip end portion of the beam member 8
and a permanent magnet 6 provided between the connecting yokes 56,
57. Further, the connecting yoke 46 provided on the base end side
is fixed to a supporting portion 47 and a coil spring 91 is
provided on the lower side of the connecting yoke 57.
The magnetostrictive rod 2 and the coil 3 used in this embodiment
may be same as the magnetostrictive rod 2 and the coil 3 used in
the first embodiment.
The beam member 8 is formed of a magnetic material and has a
function of generating the stress in the magnetostrictive rod
2.
A constituent material for the beam member 8 may be the same
material as the above-mentioned various materials to be used for
forming the first block bodies 4 and the second block bodies 5 in
the described first embodiment.
Further, it is preferable that an average thickness of the beam
member 8 is substantially equal to the thickness of the beam member
73 in the described first embodiment.
The connecting yoke 46 connects the base end portion 21 of the
magnetostrictive rod 2 and the base end portion of the beam member
8.
Upper and lower slits 461, 462 are formed on the connecting yoke 46
so as to extend along a width direction of the connecting yoke 46.
The base end portion 21 of the magnetostrictive rod 2 is inserted
into the lower slit 461 of the connecting yoke 46 and the base end
portion of the beam member 73 is inserted into the upper slit 462
of the connecting yoke 46 to fix the magnetostrictive rod 2 and the
beam member 73 to the connecting yoke 46.
A base end portion of the connecting yoke 46 is fixed to the
supporting portion 47.
The supporting portion 47 has a plate-like shape. Further, a groove
portion 471 is formed in a substantially central portion of the
supporting portion 47 on the tip end side thereof so as to pass
through the supporting portion 47 in a width direction thereof. The
connecting yoke 46 is inserted into this groove portion 471 to fix
the connecting yoke 46 to the supporting portion 47.
In the power generator 1 according to this embodiment, the base end
portion of the supporting portion 47 is fixed to a housing 100 of a
vibrating body to support the magnetostrictive rod 2 in a
cantilevered state that the base end portion 21 of the
magnetostrictive rod 2 serves as a fixed end portion and the tip
end portion 22 of the magnetostrictive rod 2 serves as a movable
end portion.
The connecting yoke 56 is provided on the tip end side of the beam
member 8.
A slit 561 is formed on a substantially central portion of the
connecting yoke 56 in a thickness direction thereof so as to extend
along a width direction of the connecting yoke 56. The tip end
portion of the beam member 8 is inserted into this slit 561 to fix
the connecting yoke 56 to the beam member 8.
The connecting yoke 57 is provided on the tip end side of the
magnetostrictive rod 2.
A slit 571 is formed on a substantially central portion of the
connecting yoke 57 in a thickness direction thereof so as to extend
along a width direction of the connecting yoke 57. The tip end
portion 22 of the magnetostrictive rod 2 is inserted into this slit
571 to fix the connecting yoke 57 to the magnetostrictive rod
2.
The permanent magnet 6 is provided between the connecting yokes 56,
57.
The permanent magnet 6 has a columnar shape. A constituent material
for the permanent magnet 6 may be same as the constituent material
for the permanent magnets 6 in the described first embodiment.
In this embodiment, the permanent magnet 6 is arranged so that its
south pole is directed toward the side of the connecting yoke 56
and its north pole is directed toward the side of the connecting
yoke 57 as shown in FIG. 13. With this configuration, it is
possible to form a magnetic field loop circulating in the clockwise
direction in the power generator 1.
In the power generator 1 according to this embodiment, the
connecting yokes 56, 57 and the permanent magnet 6 serve as a
weight for applying external force or vibration to the
magnetostrictive rod 2. When the vibrating body vibrates, external
force or vibration in the vertical direction in FIG. 13 is applied
to these components. By applying the external force or the
vibration to these components, the tip end portion 22 of the
magnetostrictive rod 2 begins reciprocating motion in the vertical
direction in the cantilevered state that the base end portion 21 of
the magnetostrictive rod 2 serves as the fixed end portion and the
tip end portion 22 of the magnetostrictive rod 2 serves as the
movable end portion. Namely, the tip end portion 22 of the
magnetostrictive rod 2 is relatively displaced with respect to the
base end portion 21 of the magnetostrictive rod 2.
A constituent material for each connecting yoke 46, 56, 57 and the
supporting portion 47 may be the same material as the
above-mentioned various materials to be used for forming the first
block bodies 4 and the second block bodies 5 in the described first
embodiment.
The coil spring 91 is provided on the lower side of the connecting
yoke 57.
The coil spring 91 is arranged between the connecting yoke 57 and a
base body 200 (which does not vibrate) in an expanded state (that
is a state that the coil spring 91 is expanded in a longitudinal
direction thereof from a natural state). One end portion of the
coil spring 91 is fixed to a lower surface of the connecting yoke
57 and the other end portion of the coil spring 91 is fixed to the
base body 200.
In the power generator 1, the magnetostrictive rod 2 (the
connecting yoke 57) is pulled toward a lower side of a displacement
direction of the coil spring 91 (the lower direction in FIG. 13) by
the coil spring 91 as shown in FIG. 13. With this configuration,
the compressive stress is generated in the magnetostrictive rod 2.
In this embodiment, the coil spring 91 constitutes the bias stress
generating mechanism for generating the compressive stress in the
magnetostrictive rod 2 in all states (containing the natural state
and a state that the external force is applied to the power
generator 1).
Even in the case where the power generator 1 takes such a
configuration, the compressive stress is generated in the
magnetostrictive rod 2 in the natural state as is the case for the
power generator 1 of the described first embodiment. Thus, even if
the intensity of the bias magnetic field applied to the
magnetostrictive rod 2 is relatively large, it is possible to
sufficiently increase the variation amount of the magnetic flux
density in the magnetostrictive rod 2. Namely, according to the
power generator 1 of this embodiment, it is also possible to
sufficiently increase the variation amount of the magnetic flux
density in the magnetostrictive rod 2 in a wide range of
intensities of the bias magnetic field.
In this embodiment, it may be possible to take a configuration in
which the coil spring 91 in a contracted state (that is a state
that the coil spring 91 is contracted in the longitudinal direction
thereof from the natural state) is arranged between the connecting
yoke 56 and the base body 200 and the both end portions of the coil
spring 91 are respectively fixed to an upper surface of the
connecting yoke 56 and the base body 200 as shown in FIG. 14. In
such a configuration, the magnetostrictive rod 2 is pressed toward
the lower side of the displacement direction of the coil spring 91
(the lower direction in FIG. 14) by the coil spring 91. With this
configuration, the compressive stress is generated in the
magnetostrictive rod 2, thereby providing the same function and
effect as the described function and effect of the power generator
1 of this embodiment.
In this embodiment, it is possible to take a configuration in which
the coil 3 is wound around the beam member 8 instead of winding the
coil 3 around the magnetostrictive rod 2. When the magnetic flux
density in the magnetostrictive rod 2 varies, the magnetic flux
density passing through the beam member 8 also varies. Thus, it is
possible to generate the voltage in the coil 3 as is the case for
the power generator 1 having the above configuration.
For fixing and connecting each component, it is possible to use a
screwing method, a caulking method, a diffusion bonding method, a
pin pressure fitting method, a brazing method, a welding method
(such as a laser welding method and an electric welding method), a
bonding method with an adhesive agent or the like.
Further, it is also possible to use an elastic member having the
same function as the coil spring 91 instead of the coil spring 91
described above. For example, a leaf spring in the expanded state
may be used in the power generator 1 shown in FIG. 13 instead of
the coil spring 91.
The power generator 1 according to this second embodiment can also
provide the same function and effect as the function and effect of
the power generator 1 according to the described first
embodiment.
Third Embodiment
Next, description will be given to a third embodiment of the power
generator of the present invention.
FIG. 15 is a side view showing the third embodiment of the power
generator of the present invention.
Hereinafter, an upper side in FIG. 15 is referred to as "upper" or
"upper side" and a lower side in FIG. 15 is referred to as "lower"
or "lower side". Further, a right side in FIG. 15 is referred to as
"tip end side" and a left side in FIG. 15 is referred to as "base
end side".
Hereinafter, the power generator according to the third embodiment
will be described by placing emphasis on the points differing from
the power generators according to the first embodiment and the
second embodiment, with the same matters being omitted from the
description.
The power generator 1 shown in FIG. 15 has the same configuration
as the power generator 1 according to the second embodiment except
that a magnet 92 is arranged between the connecting yoke 57 and the
base body 200 instead of the coil spring 91.
As shown in FIG. 15, the magnet 92 is arranged on the base body 200
so as to be spaced apart from the connecting yoke 57 in the natural
state. Further, the magnet 92 is configured to overlap with the
connecting yoke 57 in the planar view.
This magnet 92 has a columnar shape. The magnet 92 is formed of the
same material as the constituent material for the permanent magnets
9 of the described first embodiment. The magnet 92 is arranged so
that its south pole is directed toward the side of the connecting
yoke 57 and its north pole is directed toward the side of the base
body 200.
Since the connecting yoke 57 in the power generator 1 is formed of
the magnetic material, the connecting yoke 57 is attracted toward
the lower side of the displacement direction of the
magnetostrictive rod 2 (the lower direction in FIG. 15) by the
magnet 92. With this configuration, the compressive stress is
generated in the magnetostrictive rod 2. In this embodiment, the
magnet 92 and the connecting yoke 57 (magnetic member) constitute
the bias stress generating mechanism for generating the compressive
stress in the magnetostrictive rod 2 in all states.
Even in the case where the power generator 1 takes such a
configuration, the compressive stress is generated in the
magnetostrictive rod 2 in the natural state as is the cases for the
power generators 1 of the first embodiment and the second
embodiment. Thus, even if the intensity of the bias magnetic field
applied to the magnetostrictive rod 2 is relatively large, it is
possible to sufficiently increase the variation amount of the
magnetic flux density in the magnetostrictive rod 2. Namely,
according to the power generator 1 of this embodiment, it is also
possible to sufficiently increase the variation amount of the
magnetic flux density in the magnetostrictive rod 2 in a wide range
of intensities of the bias magnetic field.
Further, although the magnet 92 is arranged so as to overlap with
the connecting yoke 57 in the planar view, it is preferable from a
point of view of preventing the lines of magnetic force generated
from the magnet 92 from interfering with the magnetic field loop
formed in the power generator 1 that the magnet 92 is arranged so
as to overlap with a part of the connecting yoke 57 on the base end
side in the planar view.
In this regard, although the magnet 92 is arranged on the base body
200 so that its south pole is directed toward the side of the
connecting yoke 57 in the power generator 1 shown in FIG. 15, the
magnet 92 may be arranged on the base body 200 so that its north
pole is directed toward the side of the connecting yoke 57.
The power generator 1 according to this third embodiment can also
provide the same function and effect as the functions and effects
of the power generators 1 according to the first embodiment and the
second embodiment.
Forth Embodiment
Next, description will be given to a fourth embodiment of the power
generator of the present invention.
FIG. 16 is a perspective view showing the fourth embodiment of the
power generator of the present invention. FIG. 17 is a side view of
the power generator shown in FIG. 16. FIG. 18 is a side view
showing another configuration example of the power generator of the
fourth embodiment of the present invention.
Hereinafter, an upper side in each of FIGS. 16 to 18 is referred to
as "upper" or "upper side" and a lower side in each of FIGS. 16 to
18 is referred to as "lower" or "lower side". Further, a right and
rear side of the paper in FIG. 16 and a right side of each of FIGS.
17 and 18 are referred to as "tip end side" and a left and front
side of the paper in FIG. 16 and a left side in each of FIGS. 17
and 18 are referred to as "base end side".
Hereinafter, the power generator according to the fourth embodiment
will be described by placing emphasis on the points differing from
the power generators according to the first embodiment to the third
embodiment, with the same matters being omitted from the
description.
The power generator 1 shown in FIG. 16 includes the two
magnetostrictive rods 2 arranged side by side, the coils 3
respectively wound around the magnetostrictive rods 2, the
connecting yoke 46 for connecting the base end portions 21 of the
magnetostrictive rods 2 with each other, a connecting yoke 58 for
connecting the tip end portions 22 of the magnetostrictive rods 2
with each other, a yoke 10 arranged along the magnetostrictive rods
2 and the two permanent magnets 6 respectively arranged between the
connecting yoke 46 and the yoke 10 and between the connecting yoke
58 and the yoke 10. Further, the connecting yoke 46 provided on the
base end side is fixed to the supporting portion 47 and the
connecting yoke 58 provided on the tip end side is fixed to a
weight portion (mass portion) 59.
In the power generator 1 according to this embodiment, the bias
stress generating mechanism is constituted of a pair of coil
springs 93 respectively provided on the front side and the rear
side of the magnetostrictive rods 2 in FIG. 17 so as to face each
other through the two magnetostrictive rods 2.
In this regard, the magnetostrictive rods 2 and the coils 3 used in
this embodiment may be same as the magnetostrictive rods 2 and the
coils 3 used in the first embodiment.
The connecting yoke 46 connects the base end portions 21 of the
magnetostrictive rods 2.
As is the case for the connecting yoke 46 of the described second
embodiment, the upper and lower slits 461, 462 are formed on the
connecting yoke 46 so as to extend along the width direction of the
connecting yoke 46. The base end portions 21 of the
magnetostrictive rods 2 are respectively inserted into the upper
and lower slits 461, 462 to fix the magnetostrictive rods 2 to the
connecting yoke 46. Further, bars 463 (a pair of bars 463) are
respectively formed on both side surfaces of the connecting yoke 46
so as to be positioned between the upper and lower slits 461,
462.
The connecting yoke 46 is fixed to the supporting portion 47 on the
base end side of the supporting portion 47. The supporting portion
47 has the same configuration as that of the described second
embodiment.
The connecting yoke 58 connects the tip end portions 22 of the
magnetostrictive rods 2.
Upper and lower slits 581, 582 are formed on the connecting yoke 58
so as to extend along a width direction of the connecting yoke 58.
The tip end portions 22 of the magnetostrictive rods 2 are
respectively inserted into the upper and lower slits 581, 582 to
fix the connecting yoke 58 to the magnetostrictive rods 2. Further,
bars 583 (a pair of bars 583) are respectively formed on both side
surfaces of the connecting yoke 56 so as to be positioned between
the upper and lower slits 581, 582.
The connecting yoke 58 is fixed to the weight portion 59 on the tip
end side of the connecting yoke 58.
The weight portion 59 has a plate-like shape. A groove portion 591
is formed in a substantially central portion of the weight portion
59 on the base end side thereof so as to pass through the weight
portion 59 in a width direction thereof. The connecting yoke 58 is
inserted into this groove portion 591 to fix the weight portion 59
to the connecting yoke 58.
The weight portion 59 and the connecting yoke 58 serve as a weight
for applying external force or vibration to the magnetostrictive
rods 2. When the vibrating body vibrates, external force or
vibration in the vertical direction in FIG. 17 is applied to the
weight portion 59 and the connecting yoke 58. By applying the
external force or the vibration to the weight portion 59 and the
connecting yoke 58, the tip end portions 22 of the magnetostrictive
rods 2 begin reciprocating motion in the vertical direction in the
cantilevered state that the base end portions 21 of the
magnetostrictive rods 2 serve as the fixed end portions and the tip
end portions 22 of the magnetostrictive rods 2 serve as the movable
end portions. Namely, the tip end portions 22 of the
magnetostrictive rods 2 are relatively displaced with respect to
the base end portions 21 of the magnetostrictive rods 2.
A constituent material for each connecting yoke 46, 58, the
supporting portion 47 and the weight portion 59 may be the same
material as the above-mentioned various materials to be used for
forming the first block bodies 4 and the second block bodies 5 in
the described first embodiment.
The yoke 10 has an elongated plate-like shape. The yoke 10 is
arranged along the two magnetostrictive rods 2 in the width
direction thereof. A constituent material for the yoke 10 may be
the same material as the above-mentioned various materials to be
used for forming the first block bodies 4 and the second block
bodies 5 in the described first embodiment.
Each of the permanent magnets 6 has a columnar shape. A constituent
material for the permanent magnets 6 may be same as the constituent
material for the permanent magnets 6 in the described first
embodiment.
In this embodiment, as shown in FIG. 16, the permanent magnet 6
arranged between the connecting yoke 46 and the yoke 10 is arranged
so that its south pole is directed toward the side of the
connecting yoke 46 and its north pole is directed toward the side
of the yoke 10. On the other hand, the permanent magnet 6 arranged
between the connecting yoke 58 and the yoke 10 is arranged so that
its south pole is directed toward the side of the yoke 10 and its
north pole is directed toward the side of the connecting yoke 58.
With this configuration, it is possible to form a magnetic field
loop circulating in the clockwise direction in the power generator
1.
The coil springs 93 are respectively provided on the front side and
the rear side of the paper in FIG. 17 so as to face each other
through the two magnetostrictive rods 2.
One end portion of each of the coil springs 93 is fixed to the bar
463 of the connecting yoke 46 in the expanded state. The other end
portion of each of the coil springs 93 is fixed to the bar 583 of
the connecting yoke 58 in the expanded state.
In the power generator 1, the connecting yokes 46, 58 are pulled by
the coil springs 93 in a direction in which the connecting yokes
46, 58 approach to each other. Namely, the base end portions 21 and
the tip end portions 22 of the magnetostrictive rods 2 are pulled
by the coil springs 93 in a direction in which the tip end portions
22 approach to the base end portions 21. With this configuration,
the compressive stress is generated in each of the magnetostrictive
rods 2. In this embodiment, the coil springs 93 constitute the bias
stress generating mechanism for generating the compressive stress
in each of the magnetostrictive rods 2 in all states.
Even in the case where the power generator 1 takes such a
configuration, the compressive stress is generated in each of the
magnetostrictive rods 2 in the natural state as is the cases for
the power generators 1 of the first embodiment to the third
embodiment. Thus, even if the intensity of the bias magnetic field
applied to the magnetostrictive rods 2 is relatively large, it is
possible to sufficiently increase the variation amount of the
magnetic flux density in each of the magnetostrictive rods 2.
Namely, according to the power generator 1 of this embodiment, it
is also possible to sufficiently increase the variation amount of
the magnetic flux density in each of the magnetostrictive rods 2 in
a wide range of intensities of the bias magnetic field.
In this embodiment, it is possible to use other elastic members for
generating the compressive stress in each of the magnetostrictive
rods 2 in the natural state instead of the coil springs 93.
For example, a wire 94 as shown in FIG. 18 can be used as the
elastic member. The power generator 1 shown in FIG. 18 has a
configuration in which the base end portions 21 of the
magnetostrictive rods 2 are connected by the supporting portion 47
and the tip end portions 22 of the magnetostrictive rods 2 are
connected by the weight portion 59. The yoke 10 is fixed to the
supporting portion 47 and the weight portion 59 on the rear side of
the paper in FIG. 18 through the two permanent magnets 6.
For example, the wire 94 is formed of a metallic wire. Both end
portions of the wire 94 are respectively fixed to fixing portions
941, 942 with a caulking method or the like. A through-hole is
formed in each of the fixing portions 941, 942 so as to pass
through each of the fixing portions 941, 942 in a thickness
direction thereof. Bars 473, 593 are respectively provided on the
supporting portion 47 and the weight portion 59. The bars 473, 593
are respectively inserted into the through-holes of the fixing
portions 941, 942 to respectively fix the fixing portions 941, 942
to the supporting portion 47 and the weight portion 59.
For example, in the power generator 1 described above, by designing
the power generator 1 so that a length of the wire 94 is shorter
than a length from a tip end portion of the supporting portion 47
to a base end portion of the weight portion 59, the base end
portions 21 and the tip end portions 22 of the magnetostrictive
rods 2 are pulled in a direction in which the tip end portions 22
approach to the base end portions 21 as is the case for the
described embodiment using the coil springs 93. With this
configuration, it is possible to generate the compressive stress in
each of the magnetostrictive rods 2 in all states.
Further, by fixing the fixing portions 941, 942 to the bars 473,
593 in a state that the wire 94 is heated by a heating treatment
and then cooling the wire 94 for generating heat-shrinking in the
wire 94, the base end portions 21 and the tip end portions 22 of
the magnetostrictive rods 2 are pulled in the direction in which
the tip end portions 22 approach to the base end portions 21.
Furthermore, in the case of using a shape-memory wire having a
length shorter than the length from the tip end portion of the
supporting portion 47 to the base end portion of the weight portion
59 as the wire 94, the fixing portions 941, 942 are first fixed to
the bars 473, 593 in a state that the wire 94 is heated and
expanded. Then, the wire 94 is cooled to a certain temperature. At
this time, since the wire 94 starts to return to an original shape,
the base end portions 21 and the tip end portions 22 of the
magnetostrictive rods 2 are pulled in the direction in which the
tip end portions 22 approach to the base end portions 21. Even in
the case of using any one of the above methods, it is possible to
generate the compressive stress in each of the magnetostrictive
rods 2.
For fixing and connecting each component, it is possible to use a
screwing method, a caulking method, a diffusion bonding method, a
pin pressure fitting method, a brazing method, a welding method
(such as a laser welding method and an electric welding method), a
bonding method with an adhesive agent or the like.
Further, in this embodiment, it is possible to take a configuration
in which the coil 3 is wound around the yoke 10 instead of winding
the coils 3 around the magnetostrictive rods 2. When the magnetic
flux density in each of the magnetostrictive rods 2 varies, the
magnetic flux density passing through the yoke 10 also varies.
Thus, it is possible to generate the voltage in the coil 3 as is
the case for the power generator 1 having the above
configuration.
The power generator 1 according to this fourth embodiment can also
provide the same function and effect as the functions and effects
of the power generators 1 according to the first embodiment to the
third embodiment.
Although the power generator of the present invention has been
described with reference to the preferred embodiments shown in the
accompanying drawings, the present invention is not limited
thereto. In the power generator, the configuration of each
component may be possibly replaced with other arbitrary
configurations having equivalent functions. It may be also possible
to add other optional components to the present invention.
For example, it may be also possible to combine the configurations
according to the first embodiment to the fourth embodiment of the
present invention in an appropriate manner.
Further, in the first embodiment, it is possible to omit one of the
two permanent magnets or replace one or both of the permanent
magnets with an electromagnet. Furthermore, it is possible to take
a configuration in which both of the permanent magnets are omitted
and the power generator generates the electric power with utilizing
an external magnetic field.
Further, it is possible to replace the permanent magnet 6 and the
magnet 92 in the second embodiment to the fourth embodiment with
electromagnets. Furthermore, it is also possible to take a
configuration in which one of the permanent magnet 6 and the magnet
92 is omitted and the power generator generates the electric power
with utilizing an external magnetic field.
Further, although each of the magnetostrictive rods and the beam
member has the rectangular cross-sectional shape in each of the
embodiments, the present invention is not limited thereto. Examples
of the cross-sectional shape of each of the magnetostrictive rods
and the beam member include a circular shape, an ellipse shape and
a polygonal shape such as a triangular shape, a square shape and a
hexagonal.
Further, although the permanent magnet in each of the embodiments
has the columnar shape, the present invention is not limited
thereto. Examples of the shape of the permanent magnet include a
square columnar shape, a plate-like shape and a triangle pole
shape.
INDUSTRIAL APPLICABILITY
According to the present invention, since the compressive stress
(contraction stress) is generated in the magnetostrictive rod in
the natural state (that is a state that external force is not
applied to the power generator), the magnetic permeability of the
magnetostrictive rod is lower than the case where the stress does
not occur in the magnetostrictive rod. Thus, in this power
generator, it is possible to increase the variation amount of the
magnetic flux density caused by the generation of the tensile
stress (stretching stress) in the magnetostrictive rod and
sufficiently increase the variation amount of the magnetic flux
density in the magnetostrictive rod when the tensile stress and the
compressive stress are alternately generated in the
magnetostrictive rod. For the reasons stated above, the present
invention is industrially applicable.
* * * * *